168 Problems €4 Solutiona on Therrncdynamica d Statistical Mechanics
If E/& >> 1, N - E/& >> 1, we have
N
r 1
=k ICE\. -In-+ "E" ( 1-- :E) ln- 'El'
1--
EN
2009
Consider a system of N non-interacting particles, each fixed in position
and carrying a magnetic moment p, which is immersed in a magnetic field
H. Each particle may then exist in one of the two energy states E = 0 or
E = 2pH. Treat the particles as distinguishable.
(a) The entropy, S, of the system can be written in the form S =
klnR(E), where k is the Boltzmann constant and E is the total system
energy. Explain the meaning of R(E).
(b) Write a formula for S(n), where n is the number of particles in the
upper state. Crudely sketch S(n).
(c) Derive Stirling's approximation for large n:
Inn! = nlnn - n
by approximating In n! by an integral.
(d) Rewrite the result of (b) using the result of (c). Find the value of
(e) Treating E as continuous, show that this system can have negative
(f) Why is negative temperature possible here but not for a gas in a
(CUSPEA)
(a) R(E) is the number of all the possible microscopic states of the
n for which S(n) is maximum.
absolute temperature.
box?
Solution:
system when its energy is E, where